The speed of the programming and erasing process is one of the main figures of
merit of an EEPROM cell. Therefore, strong electric fields are applied at the
control gate to allow FOWLER-NORDHEIM tunneling of carriers during
programming and erasing cycles. However, due to this repeated high-field
stress, trap centers in the dielectric are formed which allow trap-assisted
tunneling at low fields and thus reduce the retention time of the devices.
This additional current at low bias is known as stress-induced leakage current
(SILC) and represents one of the major reliability concerns in contemporary
EEPROM devices [196,219]. In the left part of Fig. 5.26
measured SILC after different stress times for a MOS capacitor with a dielectric
thickness of 5.5nm is shown [189]. The trap-assisted tunneling
model outlined in Section 3.8.2 yields excellent agreement with the measured
data if the trap concentration is used as a fitting parameter dependent on the
stressing time (the model parameters are stated in the figure caption). The
transition from the region of mainly trap-assisted tunneling for
V
to the region of FOWLER-NORDHEIM tunneling for
V is clearly
visible. The right part of Fig. 5.26 shows the trap occupancy
across the gate dielectric of a MOS capacitor using the gate voltage as
parameter. The regions near the gate (right) and near the substrate (left)
are only sparsely occupied. Near the gate, the emission time is much smaller
than the capture time, and near the substrate, the trap energy lies above the
electron energy in the cathode.
Some of the trapped electrons face a triangular barrier for the emission
process, giving rise to an additional peak in the trap occupancy near the gate
side (the anode) of the dielectric. This is due to the wave function
interference in the FOWLER-NORDHEIM region (the oscillations are also
observed in the emission time of the traps shown in
Fig. 3.19).
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A. Gehring: Simulation of Tunneling in Semiconductor Devices